Although glasses and amorphous materials are widespread in nature since the ancient times [1]}, [2]},
a unified and coherent theoretical framework for describing their thermodynamical and dynamical properties remains still a challenge
that attracts the attention of a wide scientific community [3]}, [4]}.
Glasses can be obtained by cooling fast enough a liquid in order to avoid crystallization.
In experiment and numerical simulations, the glass transition temperature is defined as the temperature at
which the structural relaxation time \(\tau _\alpha \)  overcomes some threshold value.
A glass can thus be seen as a fluid that does not flow anymore [5]}.
Under this perspective, static observables that are usually suitable for revealing positional order as the radial distribution function \(g(r)\)  and its Fourier transform, i.e.,
the static structure factor \(S(q)\) , do not indicate remarkable differences between the liquid and the glassy state.
